Temperature measurement with combined photo-luminescent and black body sensing techniques

ABSTRACT

High temperature range black body techniques are combined with lower temperature range photoluminescent techniques to provide an optical method and apparatus for measuring temperature over a very wide range. Among the various optical probe configurations disclosed which combine the black body and photoluminescent technologies is an optical temperature measuring probe including an elongated transparent light pipe with a black body cavity and a photoluminescent material adjacent one end of the light pipe. Signal detection and processing can be combined, and temperature measurements made by the photoluminescent technique within an overlap of the two temperature ranges can be used to calibrate measurements made in the higher range by the black body technique.

This is a division of application Ser. NO. 07/683,258, filed Apr. 10,1991, now U.S. Pat. No. 5,112,137.

BACKGROUND OF THE INVENTION

This invention relates generally to techniques of optically measuringtemperature.

Optical techniques for measuring the temperature of surfaces or othersolid objects, and fluids or other environments, are becomingincreasingly utilized in place of more traditional electricaltechniques, such as those utilizing thermocouples, thermistors orresistance thermometry devices (RTDs). An early optical technique formeasuring the temperature of surfaces was infrared radiometry. With thistechnique, the infrared energy being emitted from the surface ofinterest was measured by a non-contact technique. If the emissivity ofthe surface is known, its temperature can be calculated from theinfrared emission intensity measurement. Since it is often difficult toknow with precision the emissivity of the surface of interest, suchmeasurements are not always made with the accuracy that is desired.Further, infrared radiometry is a technique which is made useful formeasuring high temperatures but is not as useful for applicationsrequiring measurement of low temperatures.

Various other optical techniques have been suggested for measuring lowertemperatures. One such technique utilizes a liquid crystal film enclosedin a housing at a tip of an optical fiber probe designed forimplantation in biological tissue to measure its temperature. Theproportion of light directed against the sensor which is reflected by itis an indication of temperature. An example of this technique is givenin U.S. Pat. No. 4,016,761 Rozzell et al. (1977). Another technique,described in U.S. Pat. No. 4,140,393 Cetas (1979) utilizes abirefringement crystal as the temperature sensing element at the end ofan optical fiber. U.S. Pat. No. 4,136,566--Christensen (1979) reliesupon a shifting light absorption edge of a semiconductor material as afunction of temperature.

Many other types of optical temperature sensors have been proposed butthe use of a photoluminescent sensor has found the widest commercialacceptance for lower temperatures. Early photoluminescent devicescontinuously excited the sensor to luminescence and measured therelative intensities of the resulting emission in defined wavelengthbands. Implementations of this technique are described in U.S. Pat. Nos.4,448,547 - Wickersheim (1984) and 4,376,890 --Engstrom et al. (1983).

More recently, the temperature dependent decay time of photoluminescenceis utilized in temperature measuring instruments. The sensor is excitedto luminesce by directing against it a time varying excitation radiationsignal and a time varying characteristic of the resulting luminescenceis detected and processed to extract temperature information from it.Examples of this are given in U.S. Pat. Nos. Re. 31,832 --Samulski(1985) and 4,652,143 --Wickersheim et al. (1987), and U.K. Patent No.2,113,837B - Bosselmann (1986). The commercial forms of such productsform a sensor of the photoluminescent material at the end of a singleoptical fiber. Because the technique measures temperature dependentdecay time changes in luminescent intensity, rather than absolutelevels, the systems require little or no calibration in order to providemeasurements of acceptable accuracy.

The photoluminescent techniques are particularly useful for measuringfrom low temperatures (such as -100° or -200° C.) to moderately hightemperatures (300 to 500° C.). However, since the technology depends onthe phenomenon of thermal quenching of luminescence, the sensormaterials cease emitting light at very high temperatures. There are avery small number of photoluminescent materials which can be used up to1000° C. or so but these materials have a very limited range of use andcannot be used at much lower temperatures.

As a separate body of technology, fiber optic probe temperature sensorshave also been developed utilizing black body structures as sensors.Examples of this technology are given in U.S. Pat. Nos. 4,576,486 --Dils(1986), 4,750,139 --Dils (1988), and 4,845,647 Dils et al. (1989).Designed primarily for measuring extremely high temperatures, anoptically transmitting probe that can withstand those temperatures iscoated at one end with an appropriate opaque material to form a blackbody cavity. Temperature dependent infrared emission from the black bodycavity is carried along the optical transmission medium to a connectingoptical fiber and then to a measuring instrument. Alternatively, anexternal object or surface can be made into the shape of a black bodycavity and a light pipe used to gather, with or without use of a lenssystem, its emissions for transmission to a detector without contactingthe black body.

While such an infrared system, when used with appropriate near infrareddetectors and transmitting materials, can also cover a wide temperaturerange, it does not work well at lower temperatures (e.g. below about200° C. to 300° C.) and thus cannot be used down to most ambienttemperatures. In order to remedy this low temperature limitation to someextent, an electrical technology, such as one using thermocouples, issometimes used in combination with the black body sensor, an awkwardcombination of optical and non-optical temperature measurementtechnologies.

Furthermore, while the black body emission follows very well definedlaws of physics in terms of its dependence on temperature, the emissionis modified by other factors, such as losses in connectors and thetransmitting materials. Since the system depends on an intensitymeasurement, calibration of the complete system is required. This is notalways convenient or possible, especially in industrial process controlor aerospace applications, where the optical transmission cables arebuilt into the system in advance and the sensors may be quite remote andtypically inaccessible.

It is a principal object of the present invention to provide an opticalsystem for accurately measuring temperatures over a very broadtemperature range. It is another object of the present invention toprovide such a system which is essentially self-calibrating.

SUMMARY OF THE INVENTION

This and additional objects are accomplished by the present invention,wherein, briefly and generally, the photoluminescent and black bodytechnologies are combined to form single sensors and accompanyingmeasuring instruments which together provide the capability for coveringa wide, continuous temperature measurement range. The sensor can eitherbe part of a probe at the end of an optical transmission medium or in aform to be attached to an object or placed in an environment with itstemperature being remotely measured without contact with a light pipe orother optical elements. Depending upon a choice of materials for thesensor, a system utilizing the present invention will accurately measureover a temperature of from -200° C. to 1000° C. or more. A specificapplication of such a technology and system is in aircraft or aerospacevehicles where temperatures range from the extremely cold ambienttemperatures of outer space to the very high temperatures generatedwithin a jet engine or at the nose of a reentry vehicle upon reenteringthe earth's atmosphere.

The present invention combines the advantages of two dissimilar opticaltechniques to produce a single system which is essentiallyself-calibrating and can measure temperature over an even wider range,such as from cryogenic temperatures to temperatures at which the sensorsbecome highly incandescent. The sole requirement is that the sensor andprobe materials can survive the desired upper temperature range withoutphysical damage or change of the optical characteristics upon which themeasurements are based. Fortunately, such materials exist and can bemade use of in such a hybrid system.

Additional objects, advantages and features of the various aspects ofthe present invention will become apparent from the followingdescription of its preferred embodiments, which description should betaken in conjunction with the accompanying drawings.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 conceptually illustrates the combination of photoluminescent andblack body temperature measuring techniques;

FIGS. 2 and 4 show exemplary black body sensor characteristics;

FIGS. 3 and 5 show exemplary photoluminescent sensor characteristics;

FIG. 6 shows the cooperative effect of the photoluminescent and blackbody measurements in order to provide temperature readings over anexpanded, continuous range of temperatures;

FIGS. 7-13 illustrate, in partial cross-sectional views, variousdifferent specific examples of temperature sensing probes combiningluminescent material and a black body structure;

FIGS. 14 and 15 show, in partially cross-sectional views, examples oftemperature sensing probes utilizing the photoluminescent materialitself to form a black body cavity;

FIGS. 16 and 17 illustrate different specific arrangements for remotelymeasuring temperature;

FIG. 18 generally illustrates one form of optical detection and signalprocessing;

FIG. 19 shows another example of optical detection and signalprocessing;

FIG. 20 shows a further example of optical detection and signalprocessing; and,

FIG. 21 shows a front view of a dual detector utilized in the embodimentof FIG. 20.

DESCRIPTION OF THE PREFERRED EMBODIMENTS

Referring initially to FIG. 1, the technique of combiningphotoluminescent and black body temperature measuring techniques isgenerally illustrated. Placed in an environment 11 whose temperature isto be measured, are two temperature measuring probes, one including aphotoluminescent sensor 13 attached to an end of an opticallytransmitting fiber or light pipe 15, and the other having a black bodysensor 17 carried by the end of an optically transparent fiber or lightpipe 19. The materials of these probes must, of course, be able towithstand the effects of a full temperature range to be measured. Thelight pipes 15 and 19 are generally selected to be sapphire since theycan withstand very high temperatures, but alternate materials can beused as well. The photoluminescent probe is optically connected by anoptical fiber 21 to a measuring instrument 23, and the black body probeis connected by an optical fiber 25 to its measuring instrument 27. Eachof the photoluminescent and black body temperature measuring systems arecommercially sold separately by Luxtron Corporation, assignee of thepresent application. What is new is the cooperative use of the twotemperature measuring technologies embodied in these systems.

Before describing details of the preferred embodiments of sensors andmeasuring techniques that combine the principles of operation of thesetwo instruments, the characteristics of each of the black body andluminescent measuring techniques will be separately described. For theblack body technique, the structure of a black body cavity at the end ofan optical light pipe by depositing a film thereon is described inaforementioned U.S. Pat. No. 4,576,486, which is incorporated herein bythis reference. The light pipe's end is generally tapered, as shown fora light pipe 29 in the embodiment of FIG. 7. Coated around that end,preferably by a sputtering technique, is an appropriate black bodycavity forming layer 31, such as platinum-rhodium. The layer is made tobe thin in order to provide a fast temperature response. The cavityemits, in a direction along the length of the light pipe 29,electromagnetic radiation at the infrared end of the optical radiationspectrum. The result is an infrared optical signal 33 which is passedback to a measuring instrument that converts the intensity of theemitted radiation to temperature.

The emission of such a sensor is illustrated with the family of curvesof FIG. 2. The spectrum of emission, generally in the infrared range,and its intensity increase with increasing temperature. The signalreceived at a detector is a bandwidth limited version of what is shownin FIG. 2 since the sapphire light pipe and optical fiber link have somelimiting effect. Additionally, in one form, a silicon photodiode is usedas a detector and a narrow bandwidth optical filter around 0.95 micronwavelength is used in conjunction with it. An electrical signal outputof this photodetector is then related to the temperature of the blackbody sensor.

Example black body emission characteristics as a function oftemperature, as observed by specific optical and detector combinations,are given in the curves of FIG. 4. Curve 42 shows a typical response ofan indium-gallium-arsenide detector over about 0.8 to 1.7 microns. Curve44 illustrates a typical response of a silicon photodiode without anyfiltering other than that provided by the optical transmission mediumitself. Curve 46 shows a response of a silicon photodiode with use of afilter having a narrow bandwidth with a center wavelength of 0.95microns.

In the photoluminescent sensor structure, such as that shown in FIG. 7in one form, a powdered luminescent material forms a sensor 35 that isphysically attached to an end of a sapphire light pipe 37 which carriesoptical signals indicated at 39, an excitation signal directed towardthe sensor 35 and the temperature dependent luminescent signal travelingaway from it to a photodetector in measuring instrumentation. Apreferred photoluminescent material and temperature measuring system isdescribed in copending application Ser. No. 621,900, filed Dec. 4, 1990of Jensen et al., of common ownership with the present application,which is incorporated herein by this reference. The preferredluminescent material described in that application is a chromiumactivated yttrium-gallium garnet ("YGG"). It has an advantage in thepresent application in that it survives the temperatures at the upperend of the extended temperature range contemplated.

Referring to FIG. 3, a curve 41 indicates an absorption spectrum of thisparticular photoluminescent material, while a curve 43 provides itsresulting luminescent emission spectra. The material is excited from alight emitting diode at about 0.65 micron wavelengths, within itsabsorption spectrum. Its luminescence is detected by a siliconphotodiode after its bandwidth is narrowed around 0.75 micron by anappropriate filter. FIG. 5 shows a curve of the measured luminescentdecay time as a function of temperature of the luminescent material.

In the combined system of FIG. 1, and in the modifications of it to bedescribed below, the continuous extended temperature range capability isprovided by utilizing the photoluminescent sensor when the temperaturebeing measured is in a lower portion of this range and by the black bodysensor when in a higher portion. Since there is some overlap in thesubranges of temperature that is measurable by each of these techniques,some decision must be made when to rely on one or the other of thetemperature signals or measurements.

The curves of FIG. 6 illustrate the preferred crossover temperatures.The lower limit of the black body measurement is determined primarily bythe choice of photodetector and bandwidth limitations of the opticalsignal transmission media. Three curves 45, 47 and 49 show, fordifferent black body detector arrangements but similar types of opticalfiber transmission paths, an estimate of the noise level of theresultant detected electrical signal as a function of temperature.Similarly, the dashed curve 51 shows an estimate of such a noisefunction for the preferred photoluminescent system described above. Thelowest noise measurements will be obtainable throughout the upper andlower temperature ranges of the combined technology when the transitiontemperature between them is the temperature at which their respectiveFIG. 6 curves intersect.

For example, the curve 45 represents the use of a silicon photodiode todetect black body radiation of an optical fiber probe of the typedescribed above, without any filters being utilized. The curve 47crosses the curve 51 at about 280° C. The curve 49 represents a casewhere a similar silicon photodiode is utilized, but with the black bodyemission wavelengths being limited to a range around 0.95 micron by anarrow bandwidth optical filter. If that combination is utilized, thecrossover temperature is about 325° C. Similarly, curve 45 shows the useof an indium-gallium-arsenide black body radiation photodetector,without any filters, and the crossover point with the photoluminescentsystem under those conditions is about 160° C. However, a givencombination of photoluminescent and black body temperature sensing willhave a single cross-over temperature that can be observed automaticallyby controlling electronic processing of both signals or can simply benoted by a user of a dual system of FIG. 1. The temperature reading fromthe photoluminescent instrument 23 is relied upon when the temperatureis below the given crossover temperature of the system, and that of theblack body instrument 27 is relied upon if above that temperature.

FIG. 6 also illustrates that there is a significant range of overlapwhere temperature can be measured to a good degree of accuracy by eithersystem. The dotted line 53 of FIG. 1 indicates coupling that may occurbetween the instruments 23 and 27, either electronically or manually byan operator of separate instruments, in order to use thephotoluminescent reading within this range of overlap to calibrate theblack body instrument reading. As mentioned above, a photoluminescenttemperature measuring system based upon the temperature dependent decaytime of the luminescence requires little or no calibration. Factors thatwill affect the absolute signal level that is detected, such as theeffect of aging of light sources and detectors, varying optical couplingof connectors, changing fiber transmission, and the like, do not affectthe photoluminescent decay time measurement. But these factors do affectthe absolute intensity of the detected black body emission, so periodiccalibration of a black body instrument is required.

Such calibration is most easily accomplished in the system of FIG. 1 byplacing both the photoluminescent sensor 13 and black body sensor 17 ata common temperature within a band around the appropriate crossovertemperature indicated in FIG. 6. The reliable temperature measured bythe photoluminescent instrument 23 is then used to adjust themeasurement of the black body instrument 27. Once adjusted, the blackbody instrument 27 will then be accurate over its full subrange oftemperatures, including those that are too high for the photoluminescentsensor to operate satisfactorily. Similarly, the black body measurementcan be used to calibrate the photoluminescent measurement in this sametemperature range, should this become necessary. An example is when thephotoluminescent material changes its response characteristics somewhatas a result of being exposed to too high a temperature and the blackbody portion of the system remains accurate from a recent calibration.

The combination of separate photoluminescent and black body sensorsindicated in FIG. 7 is preferably surrounded by a high temperaturewithstanding sheath 55, such as one made from sapphire. The interior ofthe sheath can contain air or some other material that has a refractiveindex less than that of the materials (typically sapphire) forming theoptical fibers or light pipes 29 and 37. The individual light signals 33and 39 are separately detected and processed.

In order to further integrate the photoluminescent and black bodytechniques, several examples are shown in FIGS. 8-13 of a single lightpipe or light pipe, again made of sapphire in these examples, into whichboth of the black body and photoluminescent sensors are built. In FIG.8, a light pipe 57, of circular cross-section, has a circular holedrilled in an end. Into the bottom of this hole is placed a quantity ofphotoluminescent material 59 which is held in the hole by a plug 61. Theuse of luminescent material in a powdered form is usually preferredbecause such a sensor is homogeneous and reproducible but a luminescentcrystalline material can alternatively be utilized. A black body cavity,in which the luminescent material 59 resides, is formed by a coating 63of a type generally used for such purposes. Optical communicationbetween the two sensors and a measuring instrument occurs along thesingle optical light pipe 57.

A modified probe shown in FIG. 9 includes a central optical light pipe65 having a quantity of luminescent material 67 held at an end thereofby a surrounding sheath 69. On the outside of the sheath 69, at itsenclosed end and surrounding the photoluminescent material 67, is anopaque coating 71 forming the black body cavity. The refractive index ofthe sheath 69 is made to be less than that of the light pipe 65, therebyforming a cladding, if the light pipe 65 is to function properly incarrying optical signals along its length without a high level of loss.However, it is desired to provide a coupling of optical signals out ofthe sheath 71 and into the light pipe 65 adjacent its end since asignificant level of both the black body and photoluminescent radiationsignals can exist in the sheath 69. This is accomplished by rougheningmating surfaces thereof in a region adjacent the end of the light pipe65.

Since it is difficult to provide a desired difference in the refractiveindices of the adjoining light pipe 65 and sheath 69 from availablematerials that have necessary high temperature capabilities, analternative structure, shown in FIG. 10, utilizes a smaller diameterlight pipe 73 within a similar sheath 69' such that an air space 72surrounds the light pipe 73. The air space 72 acts as a cladding sinceits refractive index is much less than that of sapphire. But in order totrap a quantity of photoluminescent material 67' within the sheath 69',a cylindrically shaped, optically clear plug 75 is tightly fit withinthe sheath 69' at the end of the light pipe 73. It is also desirable inthis embodiment, as explained with respect to the FIG. 9 embodiment, toprovide roughened surfaces where the plug 75 contacts an inside surfaceof the sheath 69'. Such roughening provides improved opticalcommunication between the black body cavity formed by the layer 71' andthe photoluminescent material, on the one hand, and the optical lightpipe 73, on the other hand, through the sheath 69' and the plug 75.

Referring to FIG. 11, the ability to selectively communicate an opticalsignal through an end and side of an optical light pipe is utilized toadvantage. A light pipe or rod 77 has a black body cavity forming layer79 applied to its tip. Adjacent this coating, but outside the black bodycavity itself, is a band 81 that surrounds the light pipe 77. The band81 includes photoluminescent material. The outside of the light pipe 77in contact with the photoluminescent sensor 81 is roughened in order toallow light rays to travel

it and an interior of the light pipe 77. One advantage of the structureof FIG. 11 is that the two optical signals travel in different modesalong the light pipe 77, a black body intensity signal 83 travelingprincipally via low order (central) modes and the photoluminescentsignal traveling via higher order modes 85.

The sensor of FIG. 12 is similar to that of FIG. 11, except that aphotoluminescent material sensor 87 is attached directly to an end of alight pipe 89, effectively completing the black body cavity, theremainder of which is formed by a coating 91 in the form of a cylindersurrounding the light pipe 89 at a position adjacent its end. As before,the surface of the light pipe 89 is roughened where the black bodycoating 91 exists. In this case, the lower order (central) modes 93contain most of the signal from the luminescent sensor 87 while highermodes 95 contain most of the signal from the black body cavity.

The sensor embodiment of FIG. 13 takes advantage of the fact that asatisfactory photoluminescent material can be made from sapphire. Ruby,previously suggested for use as a photoluminescent temperature sensor,is formed by doping sapphire with chromium. The usual sapphire opticallight pipe 97, in the embodiment of FIG. 13, has chromium diffused intoit within a black body cavity. As indicated in FIG. 13 by the varyingdensity of dots at the end of the light pipe 97, the concentration ofdopant is the highest at the light pipe's end, and then decreases zero adistance from its end. A black body cavity forming layer 101 of theusual type is then positioned over the end of the light pipe 97.Alternatively, the dopant can form a sufficient black body cavity byitself

In the embodiments of FIGS. 8-13 just described, the temperature sensingprobe utilizes separate elements to form the photoluminescent and blackbody sensors. In the embodiments of FIGS. 14 and 15, on the other hand,the luminescent material itself is shaped to form the walls of a blackbody cavity. In FIG. 14, an outer sheath 103 that is closed at one endcontains an optically transparent cone-shaped insert 105 that isoptically coupled to a light pipe 107. Packed in the space between thecone 105 and an inside surface of the sheath 103 is a quantity 109 ofphotoluminescent material. No separate coating is necessary to form ablack body cavity since that is formed by the cone-shaped element 105.

A similar result is obtained by the embodiment of FIG. 15, but with adifferent structure. A cylindrically shaped layer 111 ofphotoluminescent material is trapped between an outer sheath 113 and aninner sheath 115. A black body cavity is thus formed within the innersheath 115 at its end. An optical light pipe 117 is positioned tocommunicate with the black body cavity and thus also with thephotoluminescent material which forms its walls.

In the sensor embodiments described above, both of the photoluminescentand black body sensors are physically attached to a light pipe thatforms part of the optical path back to the measuring instrument. Thereare applications where it is desirable to remotely make such temperaturereadings by optically communicating with a sensor that is spaced somedistance away from the light pipe or other instrument optics. Examplesof such remote temperature measurements are given in FIGS. 16 and 17.

Referring to FIG. 16, a black body cavity 129 has interior walls formedof a photoluminescent material layer 131, as part of a sensor 133. Thesensor 133 is positioned in an environment or in contact with an objectwhose temperature is to be measured. An appropriate optical system 135communicates optical signals between the cavity 129 and appropriatephotodetectors (not shown). The optics 135 also communicate excitationradiation for the photoluminescent material 131. Thus, a single cavityis formed of luminescent material, in a manner similar to that of theprobes of FIGS. 14 and 15, except that this sensor 133 is adapted forremote temperature measuring applications. In the event that aparticular structure does not provide perfect black body radiationcharacteristics, high range temperature measurements are adjusted sincethe emissivity of layer 131 can be determined.

Similarly, with reference to FIG. 17, a flat sensor 137 contains agenerally flat layer 139 of photoluminescent material. An appropriateoptical system 141 allows optical signals to be communicated between thesurface 139 and the appropriate luminescent excitation source and one ormore photodetectors (not shown). The high temperature subrange of theextended temperature range being measured is accomplished by detectingthe infrared emissions of the luminescent senor 139 whose emissivity isknown and can even be controlled. Knowledge of the emissivity allows itstemperature, when in the higher end of the extended range, to becalculated from its infrared emissions. By use of a controlled sensor137, rather than sensing the infrared emissions from the surface of anobject to be measured, the emissivity can be known with some certaintyand the temperature thus measured with some accuracy. This approachfurther supplements the cross-calibration which is possible in theoverlap of the two portions of the temperature range than can bemeasured by the sensor 127.

FIGS. 18-21 illustrate generally three different ways of processing theoptical signals from the combined photoluminscent and black body sensorsdescribed previously. Referring first to FIG. 1, an optical fiber 143can communicate, for this detecting embodiment, with any of the sensorsof FIG. 8-10, and 13-17. A light source 145 emits an excitation beam 147through a beam splitter 149 and into the optical fiber 143. The lightsource 145 can be a light emitting diode, flashlamp, laser, or othertype, depending upon the characteristics of the photoluminescentmaterial to be excited A single optical signal 151 traveling through thefiber 143 from one of those sensors is divided into different frequencybands by utilizing a dichroic type of beam splitter 149. Reflecting ontoa detector 153 is a portion 155 of the light signal 151 that is longerin wavelength than about 0.95 microns. This is the wavelength range inwhich the emissions of the black body sensor lie. Another component 157of the signal 151 is directed onto another photodetector 159, thisincluding the wavelengths below 0.95 microns, which include theluminescent wavelength band example described above. An instrument 161generates a time varying signal that periodically excites theluminescent material, and also contains processing circuits for thesignal from the photodetector 159. Similarly, processing circuit 163receives the black body signal output of the detector 153 and processesthat to obtain temperature information. The instruments 161 and 163 arecooperatively operated through a link 162, which can be accomplished byhand control of two separate instruments for calibration and the like orintegration of the two through electronic circuits.

The system of FIG. 19 similarly operates with the same sensors as doesthe system of FIG. 18, but is somewhat simplified in that a temperaturecontaining optical signal 165 is not divided into its frequencycomponents but rather is directed onto a single photodetector 167. Theoutput of the photodetector 167 is supplied to both a circuit 169 fordetermining temperature from the luminescent component and a circuit 171for determining temperature from the black body component. For a givensensor temperature, the black body infrared signal is constant while theluminescent signal is time varying, so can be individually detectedGenerally, except at a calibration temperature, one or the othermeasuring systems is used but not both. Thus, the circuits -69 look atthe varying part of the optical signal and the circuits 171 look at adirect current component. Another circuit 173 provides a time varyingsignal to drive a light source 175 to provide photoluminescentexcitation radiation 177. Interconnecting circuits 170 allow forautomatic calibration of the black body measurement sub-system 171 fromreadings taken by the luminescent measurement subsystem 169 in anoverlap of the two ranges.

The processing generally illustrated by FIGS. 20 and 21 is speciallyadapted for use with the sensors of FIGS. 11 and 12. An optical signalfrom the sensor through an optical fiber 179 is imaged by appropriateoptics onto a detector structure 181 without separating wavelengthbands. A beam splitter 183 is utilized for directing into the fiber 179luminescent excitation radiation from a light source 185. The detectorstructure 181 includes a central photodetector 187 and an outer array ofphotodetector 189 arranged in a circle around it and having dimensionsthat match the peaks of the spatially separated modes outputted from thelight pipes 77 and 89 in the respective embodiments of FIGS. 11 and 12.Alternatively, the photodetector structure can be formed by a largediameter circular detector having the smaller circular detector 187positioned in front of it in a manner to function as a mask and leave anouter ring of the larger detector exposed to function as the ring 189 inthe FIG. 21 embodiment. Optical elements can be added in cooperationwith each detector to conform to the individual system in which thedetector assembly is a part.

A signal from the outer detector ring 189 is applied to a luminescentsignal processing circuit 191 and the central photodetector output isapplied to a black body signal processing circuit 193. Interconnectingcircuits 192 allow for cooperative operation including calibration. Itwill be recognized that this arrangement matches that of the FIG. 12embodiment sensor. For the FIG. 11 embodiment, the connection of the twophotodetectors with the processing circuits 191 and 193 is simplyreversed. In either case, a circuit 195 exists for driving the lightsource 185 with a time varying signal.

Although the various aspects of the present invention have beendescribed with respect to its preferred embodiments and specificexamples thereof, it will be understood that the invention is entitledto protection within the full scope of the appended claims.

It is claimed:
 1. An optical temperature measuring sensor, comprising:anelongated substantially optically transparent light pipe, a black bodycavity held adjacent one end of the light pipe and adapted to sendtemperature dependent optical emissions thereof along said light pipe,and a quantity of photoluminescent material held adjacent said one lightpipe end and adapted to send, when excitation radiation is directedthereagainst along said light pipe, temperature dependent opticalemissions thereof along said light pipe.
 2. The sensor of claim 11wherein said light pipe is made of sapphire and said photoluminescentmaterial is formed by a diffusion of chromium activator therein.
 3. Thesensor of claim 11 wherein the black body cavity is optically coupledwith said light pipe through said one end thereof and thephotoluminescent material is optically coupled with said light pipethrough a side surface thereof adjacent said one end.
 4. The sensor ofclaim 11 wherein the photoluminescent material is optically coupled withsaid light pipe through said one end thereof and the black body cavityis optically coupled with said light pipe through a side surface thereofadjacent said one end.
 5. The sensor of claim 11 wherein said black bodycavity is formed by a coating of opaque material carried by said onelight pipe end and extending a distance therefrom along the light pipe,and wherein said quantity of photoluminescent material is positionedwithin said cavity.
 6. The sensor of claim 1 wherein said black bodycavity includes walls formed of said quantity of photoluminescentmaterial.